Optical isolator with optical fibers arranged on one single side

ABSTRACT

An optical isolator has optical fibers arranged on a single side. The optical isolator includes an input optical fiber, an output optical fiber, an input splitting/combining device, an output splitting/combining device, an input optical rotation device, an output optical rotation device, a lens, a Faraday rotator, and a reflector. The input optical fiber and the output optical fiber are on a same side of each of the lens, the Faraday rotator, and the reflector. The optical isolator with input and output optical fibers arranged on a single side only needs to use one lens. The input and output splitting/combining devices are fixed on an end surfaces of input/output optical fibers, respectively.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims priority to Chinese Patent Application No.202010046874.6 filed on Jan. 16, 2020, the content of which is reliedupon and incorporated herein by reference in its entirety.

TECHNICAL FIELD

The disclosure relates generally to passive optical devices used in thefield of optical fiber communications, in particular to an opticalisolator with optical fibers arranged on one single side.

BACKGROUND

In an optical fiber communication system, reverse light from endsurfaces of optical fibers and nodes can exists to various degrees on atransmission line or path. Such reverse light affects the normal outputof a laser and causes, for example, fluctuating intensity, frequencydrift, decreased modulation bandwidth, and increased noise. These maydisrupt normal operations of the laser. Meanwhile, such reverse lightmay also cause the transmission performance of the system todeteriorate, may cause an optical amplifier to undergo gain change andgenerate auto-excitation, and may further result in error code.

An optical isolator is a non-reciprocal device that only allows one-waytransmission of light. An optical isolator can suppress the transmissionof reverse light, can reduce the damage caused by reverse light to alaser, can maintain the operating stability of the laser, and can extendthe service life of the laser. Therefore, as an important passiveoptical device, optical isolators are broadly used in high-speed andlarge-capacity optical fiber communication systems.

With the technical development in the entire communication industry, itwill continue to be an important trend of the technical development tominiaturize and lower the cost of passive optical devices, which is notonly a demand by the technical development of the industry, but also anurgent demand from the market. Mainstream optical isolators currently onthe market are a type of device that has optical fibers arranged on twosides and that adopts a dual-collimator structure. Accordingly, theoverall size is affected by the size of collimators. The requiredassembly space is large, and material costs are high. Further, as theinput and output optical fibers are located on two sides of the device,the optical fibers on two sides need to be organized separately when thedevice is used on or as a module for cascade connection with otherdevices. Accordingly, the process is relatively complex.

SUMMARY

The present disclosure is directed to an optical isolator with opticalfibers arranged on one single side, so as to have a small structuralsize, low cost, and simple assembly process.

In one aspect, an optical isolator may include optical fibers arrangedon a single side. The optical isolator may include an input opticalfiber, an output optical fiber, an input splitting/combining device, anoutput splitting/combining device, an input optical rotation device, anoutput optical rotation device, a lens, a Faraday rotator, and areflector that are sequentially arranged. The Faraday rotator includes amagneto-optical crystal and a magnetic field device. End surfaces of theinput optical fiber and the output optical fiber close to the lens arelocated in the same plane. The input splitting/combining device and theinput optical rotation device correspond to the input optical fiber andare sequentially fixed on the end surface of the input optical fiber andbeing close to the lens. That is, the input splitting/combining deviceis fixed on the input optical fiber, and the input optical rotationdevice is fixed on the input splitting/combining device. The outputsplitting/combining device and the output optical rotation devicecorrespond to the output optical fiber and are sequentially fixed on theend surface of the output optical fiber and being close to the lens.That is, the output splitting/combining device is fixed on the outputoptical fiber, and the output optical rotation device is fixed on theoutput splitting/combining device. There are two focal planes on twoouter sides of the lens. Transmission end surfaces of the input opticalfiber and the output optical fiber are located on a first focal plane ofthe lens, and the reflecting face of the reflector is located on asecond focal plane of the lens. The Faraday rotator is located betweenthe lens and the reflector.

In some examples, when an incident beam is inputted from the inputoptical fiber, the beam passes the input splitting/combining device tobe split, further enters the input optical rotation device for opticalrotation, subsequently irradiates into the lens to form a collimatedbeam, passes through the Faraday rotator for optical rotation,irradiates into the reflector and is reflected, returns to the Faradayrotator for optical rotation, further irradiates into the output opticalrotation device for optical rotation, further enters the outputsplitting/combining device to be combined, and enters the output opticalfiber to be output.

In certain examples, an incident beam is inputted from the outputoptical fiber, the beam passes the output splitting/combining device tobe split, further enters the output optical rotation device for opticalrotation, subsequently irradiates into the lens to form a collimatedbeam, passes through the Faraday rotator for optical rotation,irradiates into the reflector and is reflected, returns to the Faradayrotator for optical rotation, further irradiates into the input opticalrotation device for optical rotation, further enters the inputsplitting/combining device and cannot be combined, and output isolationon the input optical fiber is performed.

As an example implementation, furthermore, the number of the inputoptical fibers is equal to the number of the output optical fibers andis 2N, where N is an integer greater than 1. The input optical fibersand the output optical fibers are combined into a porous optical fiberhead or an optical fiber array, and the input optical fibers and theoutput optical fibers are arranged and combined into a structure that issymmetric with respect to a center.

In some examples, the input splitting/combining device and the outputsplitting/combining device include a displacement-type birefringentcrystal and are used for splitting/combining the o light and the e lightinside the crystal. An optical axis of the birefringent crystalintersects obliquely with a surface of the crystal. A splittingdirection of the o light and the e light is perpendicular to the beampropagation direction and is parallel to the direction of relativedisplacement between the input optical fiber and the output opticalfiber.

In some examples, the angle between optical axes of the birefringentcrystal and incident wavevector is around 45 degrees, and the splittingdistance between the o light and the e light is increased. e.g., to amaximum value, when the crystal has a consistent thickness.

In certain examples, the optical axes of the input splitting/combiningdevice and the output splitting/combining device have the same directionor are perpendicular to each other; and the input splitting/combiningdevice and the output splitting/combining device may be a plurality ofindependent devices or may be integrally formed into the same device.

In another example, the input optical rotation device and the outputoptical rotation device include a ½ wavelength (λ) phase delay-typecrystalline quartz waveplate used for rotating a polarization directionof a linear polarized light; and the optical axes of the input opticalrotation device and the output optical rotation device intersectobliquely with a surface of the crystals. A combination of the inputoptical rotation device and the output optical rotation device performsa total rotation angle of 45 degrees for the polarization direction ofthe linear polarized light.

In yet another example, the optical rotation angle of the input opticalrotation device is 0 degree, and the optical rotation angle of theoutput optical rotation device is 45 degrees; or, the optical rotationangle of the input optical rotation device is 45 degrees, and theoptical rotation angle of the output optical rotation device is 0degree.

In some example, the rotation angle of the optical rotation devices is45 degrees, and the angle between the optical axes thereof and an edgeof a crystal surface is 67.5 degrees or 22.5 degrees. In certainexamples, the rotation angle of the optical rotation devices is 0degree, and the angle between the optical axes thereof and an edge of acrystal surface is 0 degree or 90 degrees.

In another example, the lens is a C lens or other lens having focalplanes on two sides used for focalizing and collimating light beams.

In yet another example, the Faraday rotator is used for rotating apolarization direction of a linear polarized light, and the rotationangle thereof is 22.5 degrees.

In some examples, the Faraday rotator may be a combination of amagneto-optical crystal and a magnetic field device or may also be anindependent magneto-optical crystal.

In certain examples, the magnetic field device is a permanent magnet,such as a magnetic ring or parallel plates made of a magnetic materialused for providing a saturated magnetic field strength for themagneto-optical crystal, causing the magneto-optical crystal to performfixed rotation of the polarization direction of the linear polarizedlight. The magnetic field direction may be parallel to the lightpropagation direction.

In another examples, when the linear polarized light incomes from an Npole of the magnetic field, the polarization direction is rotatedclockwise viewing along a direction opposite the light propagationdirection; and when the linear polarized light incomes from the S poleof the magnetic field, the polarization direction is rotatedcounterclockwise viewing along a direction opposite the lightpropagation direction.

In yet another example, when the optical axes of the inputsplitting/combining device and the output splitting/combining devicehave the same direction, the input optical rotation device, the outputoptical rotation device, and the Faraday rotator are combined to performa total rotation angle of 90 degrees for a linear polarized light duringforward input and a total rotation angle of 0 degree for the linearpolarized light during backward input. In some examples, when theoptical axes of the input splitting/combining device and the outputsplitting/combining device perpendicular to each other, the inputoptical rotation device, the output optical rotation device, and theFaraday rotator are combined to perform a total rotation angle of 0degree for the linear polarized light during forward input and a totalrotation angle of 90 degrees for the linear polarized light duringbackward input.

In some examples, the reflector is a glass sheet having a certainthickness, and the reflection surface thereof is coated with a highlyreflective film.

By adopting the above-described technical solutions, the presentdisclosure uses a reflector to turn the light, such that the deviceneeds to use only one collimator, which, as compared with existingisolators, eliminates one collimator, reduces the device volume by half,reduces the space required for assembly inside the module by half, andaccordingly lowers the material cost. Further, the input and the outputof the present solution are on the same side of the device, andsingle-side fiber organizing may be performed at the same time as theassembly inside the module, which simplifies the process of fiberorganizing and assembly. Further, by fixing the splitting/combiningdevices on end surfaces of the input/output optical fibers, control ofinput/output and function scalability may be improved. Further, therequired volume of splitting/combining devices may be reduced, leadingto a more compact structure and lower material cost.

BRIEF DESCRIPTION OF THE DRAWINGS

The present disclosure will be further described in detail below withreference to embodiments and accompanying drawings in which:

FIG. 1 is a perspective view of an optical isolator having opticalfibers arranged on a single side according to various embodiments of thepresent disclosure;

FIG. 2 is a side view on an X-Z plane of the optical isolator of FIG. 1having the optical fibers arranged on the single side according tovarious embodiments of the present disclosure:

FIG. 3 is another side view on an Y-Z plane of the optical isolator ofFIG. 1 having the optical fibers arranged on the single side accordingto various embodiments of the present disclosure;

FIGS. 4A and 4B are schematic diagrams of an assembled structure ofsplitting/combining devices and optical rotation devices of the opticalisolator of FIG. 1 according to various embodiments of the presentdisclosure;

FIG. 5 is a schematic structural diagram of an example Faraday rotatoraccording to various embodiments of the present disclosure;

FIG. 6 illustrates an X-Z plane schematic diagram of the opticalisolator of FIG. 1 showing an example forward light path according tovarious embodiments of the present disclosure;

FIG. 7 illustrates an X-Z plane schematic diagram of the opticalisolator of FIG. 1 showing an example backward light path according tovarious embodiments of the present disclosure;

FIG. 8 illustrates an Y-Z plane schematic diagram of the opticalisolator of FIG. 1 showing an example light path according to variousembodiments of the present disclosure:

FIG. 9 illustrates a side view on an X-Z plane of another opticalisolator having optical fibers arranged on a single side according tovarious embodiments of the present disclosure;

FIG. 10 illustrates another side view on an Y-Z plane of the opticalisolator of FIG. 9 having the optical fibers arranged on the single sideaccording to various embodiments of the present disclosure;

FIGS. 11A and 11B are schematic diagrams of an assembled structure ofsplitting/combining devices and optical rotation devices of the opticalisolator of FIG. 9 according to various embodiments of the presentdisclosure:

FIG. 12 illustrates an X-Z plane schematic diagram of the opticalisolator of FIG. 9 showing an example forward light path according tovarious embodiments of the present disclosure;

FIG. 13 illustrates another X-Z plane schematic diagram of the opticalisolator of FIG. 9 showing an example backward light path according tovarious embodiments of the present disclosure;

FIG. 14 illustrates an Y-Z plane schematic diagram of the opticalisolator of FIG. 9 showing an example light path according to variousembodiments of the present disclosure;

FIG. 15 illustrates an X-Z plane schematic diagram of yet anotherexample optical isolator showing an example forward light path accordingto various embodiments of the present disclosure; and

FIG. 16 illustrates another X-Z plane schematic diagram of the opticalisolator of FIG. 15 showing an example backward light path according tovarious embodiments of the present disclosure.

DETAILED DESCRIPTION

As shown in FIGS. 1 to 3, an optical isolator 100 of the presentdisclosure includes an input 10, an output 20, an inputsplitting/combining (e.g., birefringent) device 30, an outputsplitting/combining (e.g., birefringent) device 40, an input opticalrotation device 50, an output optical rotation device 60, a lens 70, anintermediate rotation device (e.g., Faraday rotator) 80, and a reflector90 that are sequentially arranged.

As shown in FIGS. 1 to 3, the input 10 and output 20 can include aninput optical fiber 10 and an output optical fiber, and the inputoptical fiber 10 and the output optical fiber 20 can be combined into adual optical fiber head (DOFH) 15. The input optical fiber 10 and theoutput optical fiber 20 are symmetrically distributed with respect to anaxis of the DOFH 15 along X-direction; and have the same position in theY direction. The number of the input optical fiber 10 may be one, andthe number of the output optical fiber 20 may be one, so as to performthe function of one in and one out for the isolator 100.

Other arrangements can be used. For example, one or more input opticalfibers (e.g., 10) and one or more output optical fibers (e.g., 20) maybe combined in a porous optical fiber head or an optical fiber array forpositioning the optical fibers, or may be positioned using any othersuitable structures. An optical fiber head may include, for example,optical fibers and a glass structures for positioning the opticalfibers.

The input splitting/combining device (e.g., 30) and the outputsplitting/combining device (e.g., 40) may be independent devices or maybe integrally formed into the same device. The input optical rotationdevice (e.g., 50) and the output optical rotation device (e.g., 60) maybe independent devices or may be integrally formed into the same device.

End surfaces of the input optical fiber 10 and the output optical fiber20 are located in the same plane. The input splitting/combining device30 is fixed on the input optical fiber 10, and the input opticalrotation device 50 is fixed on the input splitting/combining device 30.The lens 70 has two focal planes on outer sides of the lens 70. The endsurfaces of the input optical fiber 10 and the output optical fiber 20are located on a first focal plane 71 of the lens 70, and the reflectingface of the reflector 90 is located on a second focal plane 72 of thelens 70. The Faraday rotator 80 is located between the lens 70 and thereflector 90. The output splitting/combining device 40 is fixed on theoutput optical fiber 20. The output optical rotation device 60 is fixedon the output splitting/combining device 40.

As shown in FIGS. 4A and 4B, in some embodiments, the inputsplitting/combining device 30 and the output splitting/combining device40 may include, for example, Yttrium Vanadate (YVO₄) crystals, which aredisplacement-type birefringent crystal and used for splitting/combiningthe o-light (i.e., ordinary ray) and the e-light (i.e., extraordinaryray) inside the crystal. As expected, the o-light behaves according toSnell's law while the e-light does not. The input splitting/combiningdevice 30 and the output splitting/combining device 40 may be mutuallyindependent; and may be used for splitting or combining the o light(e.g., ordinary light) and the e light (e.g., extraordinary light)inside the crystals, e.g., splitting the o-light from the e light orcombining the o light (e.g., ordinary light) and the e light. In someexamples, an optical axis 31 of the input splitting/combining device 30and an optical axis 41 of the output splitting/combining device 40 havethe same direction.

In general, the optical axis (31, 41) may intersect obliquely with anedge (33, 43) of a surface (32,42) of the crystal (30,40) at an angle of45 degrees. For example, the optical axis 31 may be in or parallel tothe surface 32 of the crystal 30, and an angle A31 between the opticalaxis 31 and the edge 33 (e.g., along +X direction) of the surface 32 ofthe crystal 30 may be 45 degrees; and the optical axis 41 may be in orparallel to the surface 42 of the crystal 40, an angle A41 between theoptical axis 41 and the edge 43 (e.g., along +X direction) of thesurface 42 of the crystal 40 may be 45 degrees. The splitting directionof the o light and the e light is perpendicular to the beam propagationdirection (the Z direction) and is parallel to a direction of relativedisplacement (the X direction) between the input optical fiber 10 andthe output optical fiber 20. That is, the splitting direction of the olight and the e light is along the X direction.

As shown in FIGS. 4A and 4B, in some embodiments, the input opticalrotation device 50 and the output optical rotation device 60 may includea half-wave plate used for rotating a polarization direction of a linearpolarized light. For example, the optical rotation devices 50, 60 can bea type of ½ wavelength (λ) phase delay-type crystalline quartzwaveplates used for rotating a polarization direction of a linearpolarized light. An angle between the optical axis 51 of the inputoptical rotation device 50 and the X axis is 0 degree, and the rotationangle of a linear polarized light in the X-Y plane is 0 degree inpolarization directions, such as the X direction, the Y direction, andthe 45-degree direction. The angle between the optical axis 61 of theoutput optical rotation device 60 and the X axis is 22.5 degrees, andthe rotation angle of a linear polarized light in the X-Y plane is 45degrees in polarization directions, such as the X direction, the Ydirection, and the 45-degree direction.

In the examples of FIGS. 1 to 3, the lens 70 may be a C-lens, and mayhave two focal planes, e.g., front and back focal planes 71, 72. As istypical and as shown in FIG. 3, the C-lens 70 includes an oblique endsurface.

As shown in FIG. 5, in some embodiments, the Faraday rotator 80 includesa magneto-optical crystal 81 and a magnetic field device 82. Themagnetic field device 82 may be, for example, a hollow magnetic ringused for providing a saturated magnetic field strength for themagneto-optical crystal 82, causing the magneto-optical crystal 82 toperform a rotation of the polarization direction of the linear polarizedlight in the X-Y plane with the rotation angle at 22.5 degrees. Themagnetic field direction is parallel to the light propagation direction.That is, the magnetic field direction is in the Z direction. When thelinear polarized light incomes from the N pole 83 of the magnetic field,the polarization direction may be rotated clockwise, e.g., viewing along−Z direction.

As shown in FIG. 6, the isolator 10 allows incident light of an opticalbeam in a forward light path at the input 10 to pass for output at theoutput 20. The forward light path in the X-Z plane in this embodiment isas follows. An incident light beam is input from the input optical fiber10 (x=x0, z=z0) along the Z direction. The light beam passes the inputsplitting/combining device 30, which splits the o light and the e light(i.e., displaces the e-light relative to the o-light) in the crystal ofthe input splitting/combining device 30. That is, one incident beam issplit into two linear polarized light beams, having a first linearpolarized light beam, e light, polarized in a direction in X-Z plane andindicated by a double-headed arrow 35, and a second linear polarizedlight beam, o light, polarized in the Y direction indicated by a dot 36.The beams enter the input optical rotation device 50, and thepolarization directions of the two linear polarized light beams arerotated clockwise by 0 degree, i.e., being not rotated by the inputoptical rotation device 50, e.g., viewing along −Z direction.

From the rotation device 50, the polarized beams enter the lens 70,where beam collimation and focusing are performed. As the polarizedbeams pass the magneto-optical crystal 81 in the Faraday rotator 80, thepolarization directions of the two linear polarized light beams are thenrotated clockwise by an amount of 22.5 degrees, e.g., viewing along −Zdirection. Passing from the rotator 80, the polarized beams are focusedonto the reflection surface 91 of the reflector 90.

At the reflector 90, the polarized beams are reflected by the reflectionsurface 91 and return to or reach the magneto-optical crystal 81 in theFaraday rotator 80, and, accordingly, the polarization directions of thetwo linear polarized light beams are again rotated clockwise by the sameamount of 22.5 degrees. e.g., viewing along −Z direction. Passing fromthe rotator 80, the polarized beams enter the output optical rotationdevice 60, and the polarization directions of the two linear polarizedlight beams are rotated clockwise by 45 degrees, e.g., viewing along −Zdirection. At this point, the total rotation angle of each of the twolinear polarized light beams is 90 degrees. Therefore, the beams can becombined by further entering the output splitting/combining device 40 sothat the combined beam enters the output optical fiber 20 (x=−x0, z=z0)for outputting.

In contrast to the forward light path of FIG. 6, the isolator 100 asshown in FIG. 7 isolates incident light of an optical beam at the output20 from being output in a backward light path to the input 10. Thebackward isolation light path in the X-Z plane in this embodiment is asfollows. An incident light beam input from the output optical fiber 20(x=−x0, z=z) along the Z direction can passes to the outputsplitting/combining device 40, which splits the o light and the e lightin the crystal of the output splitting/combining device 40. That is, oneincident beam is split into two linear polarized light beams, having afirst linear polarized light beam polarized in a direction in X-Z planeand indicated by a double-headed arrow and a second linear polarizedlight beam polarized in the Y direction indicated by a dot, in thecrystal of the output splitting/combining device 40.

From the splitting/combining device 40, the polarized beams enter theoutput optical rotation device 60, and the polarization directions ofthe two linear polarized light beams are rotated counterclockwise by 45degrees, e.g., viewing along −Z direction. From the rotating device 60,the polarized beams enter the lens 70, where beam collimation andfocusing are performed. As the polarized beams pass the magneto-opticalcrystal 81 in the Faraday rotator 80, the polarization directions of thetwo linear polarized light beams are rotated clockwise by an amount of22.5 degrees, e.g., viewing along −Z direction. The beams are focusedonto the reflection surface 91 of the reflector 90.

At the reflector 90, the polarized beams are reflected by the reflectionsurface 91 and return to the magneto-optical crystal 81 in the Faradayrotator 80, and, accordingly, the polarization directions of the twolinear polarized light beams are again rotated clockwise by the amountof 22.5 degrees, e.g., viewing along −Z direction. From the lens 70, thepolarized beams enter the input optical rotation device 50, and thepolarization directions of the two linear polarized light beams arerotated clockwise by 0 degree, i.e., not being rotated by the inputoptical rotation device 50, e.g., viewing along −Z direction. At thispoint, the total rotation angle of the two linear polarized light beamsis 0 degree. Therefore, the beams are not combined after furtherentering the input splitting/combining device 30. Instead, the inputsplitting/combining device 30 further displaces the e-light relative tothe o-light. Accordingly, the input optical fiber 10 (x=x0, z=z0) has nolight beam to output.

In the example of FIG. 8, no beam splitting or combining is performed inthe Y-Z plane. The input optical fiber 10 and the output optical fiber20 are located at the same y position. The light incoming from the inputoptical fiber 10 (y=y0, z=z0) is not displaced in the Y-Z plane in itsreturn, to the output optical fiber 20 (y=y0, z=z0) for outputting.

In examples of FIG. 6, the total rotation angle of each of the twolinear polarized light beams is 90 degrees clockwise, e.g., viewingalong −Z direction, and the beam enters the output optical fiber 20 foroutputting. In other examples, the total rotation angle of each of thetwo linear polarized light beams may be 90 degrees counterclockwise,e.g., viewing along −Z direction, and the beam enters the correspondingoutput optical fiber for outputting. Altering the rotation of therotation devices and rotator can readily achieve this.

As shown FIGS. 9 to 10, in some embodiments, an optical isolator 200 ofthe present disclosure includes an input having more than one inputoptical fiber 11, 12 and includes an output having more than one outputoptical fiber 21, 22. Other features of this isolator 200 can be similarto the isolator 100 disclosed above. This isolator 200 includes an inputsplitting/combining device 30, an output splitting/combining device 40,an input optical rotation device 50, an output optical rotation device60, a lens 70, an intermediate rotation device (i.e., Faraday rotator)80, and a reflector 90 that are sequentially arranged. End surfaces ofthe input optical fiber 11, the input optical fiber 12, the outputoptical fiber 21, and the output optical fiber 22 are located in thesame plane. The input splitting/combining device 30 is fixed on theinput optical fiber 11 and the input optical fiber 12, and the inputoptical rotation device 50 is fixed on the input splitting/combiningdevice 30.

There are two focal planes on the outer side of the lens 70. Endsurfaces of the input optical fiber 11, the input optical fiber 12, theoutput optical fiber 21, and the output optical fiber 22 are located ona first focal plane 71 of the lens 70. The reflecting face of thereflector 90 is located on a second focal plane of the lens 7. TheFaraday rotator 80 is located between the lens 70 and the reflector 90.The output splitting/combining device 40 is fixed on the output opticalfiber 21 and the output optical fiber 22, and the output opticalrotation device 60 is fixed on the output splitting/combining device 40.

As shown in FIGS. 11A and 11B, in some embodiments, the input opticalfiber 11 (x1,y1), the input optical fiber 12 (x1, −y1), the outputoptical fiber 21 (−x1, −y1), and the output optical fiber 22 (−x1, y1)are combined into a four-optical-fiber head (FOFH). The input opticalfiber 11 (x1, y1) and the output optical fiber 21 (−x1, −y1) aresymmetrically distributed or arranged with respect to an axis of theFOFH. The input optical fiber 12 (x1, −y1) and the output optical fiber22 (−x1, y1) are symmetrically distributed or arranged with respect toan axis of the FOFH. The number of the input optical fibers is two, andthe number of the output optical fibers is two. Accordingly, the opticalisolator 200 can function for two inputs and two outputs.

As shown in FIGS. 11A-11B, in some embodiments, the inputsplitting/combining device 30 and the output splitting/combining device40 may include, for example, a YVO4 crystal. In some examples, the inputsplitting/combining device 30 and the output splitting/combining device40 may be mutually independent and may be used for splitting/combiningthe o light and the e light inside the crystal. An optical axis 31 ofthe input splitting/combining device 30 and an optical axis 41 of theoutput splitting/combining device 40 may have the same direction, andthe optical axes (31, 41) may intersect obliquely with a surface of thecrystal at an angle of 45 degrees. The splitting direction of the olight and the e light is perpendicular to the beam propagation direction(the Z direction) and is parallel to the direction of relativedisplacement (the X direction) between the input optical fiber 10 andthe output optical fiber 20 That is, the splitting direction of the olight and the e light is in the X direction.

As shown in FIGS. 11A and 11B, in some embodiments, the input opticalrotation device 50 and the output optical rotation device 60 may includea half-wave plate used for rotating a polarization direction of a linearpolarized light. An angle between the optical axis 51 of the inputoptical rotation device 50 and the X axis is 0 degree, and the rotationangle of a linear polarized light in the X-Y plane is 0 degree inpolarization directions, such as the X direction, the Y direction, andthe 45-degree direction. The angle between the optical axis 61 of theoutput optical rotation device 60 and the X axis is 22.5 degrees, andthe rotation angle of a linear polarized light in the X-Y plane is 45degrees in polarization directions, such as the X direction, the Ydirection, and the 45-degree direction.

As shown in FIGS. 9 to 11, the lens 70 may be a C lens, and may have twofocal planes, e.g., front (first) and back (second) focal planes 71, 72.

The Faraday rotator 80 for the isolator 200 can be similar to that shownin FIG. 5, in some embodiments, the Faraday rotator 80 includes amagneto-optical crystal 81 and a magnetic field device 82. The magneticfield device 82 may be, for example, a hollow magnetic ring used forproviding a saturated magnetic field strength for the magneto-opticalcrystal 82, causing the magneto-optical crystal 82 to perform a rotationof the polarization direction of the linear polarized light in the X-Yplane with the rotation angle at 22.5 degrees. The magnetic fielddirection is parallel to the light propagation direction. That is, themagnetic field direction is in or parallel to the +/−Z direction. Whenthe linear polarized light incomes from the N pole 83 of the magneticfield, the polarization direction may be rotated clockwise, e.g.,viewing along −Z direction or a direction opposite the light propagationdirection.

As shown in FIG. 12, the isolator 200 allows incident light of anoptical beam in a forward light path at the inputs 11, 12 to pass foroutput at the output 21, 22. The forward light path in the X-Z plane inthis embodiment is as follows. Two incident light beams are inputted,respectively, from the input optical fiber 11 (x=x1, z=z0) and the inputoptical fiber 12 (x=x1, z=z0) along the Z direction. The light beamspass the input splitting/combining device 30 to cause the splitting ofthe o light and the e light in the crystal. That is, each incident beamis split into two linear polarized light beams, having a first linearpolarized light beam polarized in a direction in X-Z plane indicated bya double-headed arrow, e.g., e light beam, and a second linear polarizedlight beam polarized in the Y direction indicated by a dot, e.g. o lightbeam. The beams enter the input optical rotation device 50, and thepolarization directions of the four linear polarized light beams arerotated clockwise by 0 degree, i.e., being not rotated by the inputoptical rotation device 50, e.g., viewing along −Z direction.

From the rotation device 50, the polarized beams enter the lens 70,where beam collimation and focusing are performed. From the rotationdevice 50, beams pass the magneto-optical crystal 81 in the Faradayrotator 80, the polarization directions of the four linear polarizedlight beams are rotated clockwise by 22.5 degrees, e.g., viewing along−Z direction. Further, the beams are focused onto the reflection surface91 of the reflector 90. The beams are reflected by the reflectionsurface 91 and return to or reach the magneto-optical crystal 81 in theFaraday rotator 80, and, accordingly, the polarization directions of thefour linear polarized light beams are then rotated clockwise by anamount of 22.5 degrees, e.g., viewing along −Z direction. Passing fromthe rotator 80, the polarized beams enter the output optical rotationdevice 60, and the polarization directions of the four linear polarizedlight beams are rotated clockwise by 45 degrees, e.g., viewing along −Zdirection. At this point, the total rotation angle of each of the fourlinear polarized light beams is 90 degrees clockwise, e.g., viewingalong −Z direction, and the beams can be combined by entering the outputsplitting/combining device 40. Accordingly, two emitting beamscorresponding to the two incident beams are formed; and the two emittingbeams respectively enter the output optical fiber 21 (x=−x1, z=z0) andthe output optical fiber 22 (x=−x1, z=z0) for outputting.

In contrast to the forward light path of FIG. 12, the isolator 200 asshown in FIG. 13 isolates incident light of an optical beam at theoutput 20 from being output in a backward light path to the input 10.The backward isolation light path in the x-z plane in this embodiment isas follows. Two incident beams input from the output optical fiber 21(x=−x1, z=z0) and the output optical fiber 22 (x=−x1, z=z0) along the Zdirection can pass to the output splitting/combining device 40, whichsplits the o light and the e light in the crystal of the outputsplitting/combining device 40. That is, each incident beam is split intotwo linear polarized light beams, having a first linear polarized lightbeam polarized in a direction in X-Z plane and indicated by adouble-headed arrow and a second linear polarized light beam polarizedin the Y direction indicated by a dot.

From the splitting/combining device 40, the beams enter the outputoptical rotation device 60, and the polarization directions of the fourlinear polarized light beams are rotated counterclockwise by 45 degrees,e.g., viewing along −Z direction. From the rotating device 60, the beamsenter the lens 70, where beam collimation and focusing are performed. Asthe beams pass the magneto-optical crystal 81 in the Faraday rotator 80,the polarization directions of the four linear polarized light beams arerotated clockwise by 22.5 degrees, e.g., viewing along −Z direction. Thepolarized beams are focused onto the reflection surface 91 of thereflector 90. The beams are reflected by the reflection surface 91 andreturn to or reach the magneto-optical crystal 81 in the Faraday rotator80, and, accordingly, the polarization directions of the four linearpolarized light beams are rotated clockwise by 22.5 degrees, e.g.,viewing along −Z direction. Further, the beams enter the input opticalrotation device 50, and the polarization directions of the four linearpolarized light beams are rotated clockwise by 0 degree, i.e., not beingrotated by the input optical rotation device 50, e.g., viewing along −Zdirection. At this point, the total rotation angle of each of the fourlinear polarized light beams is 0 degree. Therefore, the beams are notcombined after further entering the input splitting/combining device 30.Instead, the input splitting/combining device 30 further displaces thee-light relative to the o-light. Accordingly, the input optical fiber 11(x=x1, z=z0) and the input optical fiber 12 (x=x1, z=z0) have no lightbeam to output.

In the examples of FIG. 14, there is no beam splitting/combining in theY-Z plane. Light incoming from the input optical fiber 11 (y=y1, z=z0)and being focused by the lens 70 and reflected by the reflector 90enters the output optical fiber 21 (=−y1, z=zo) for outputting.Meanwhile, light incoming from the input optical fiber 22 (y=y1, z=z0)and being focused by the lens 70 and reflected by the reflector 90,enters the output optical fiber 12 (y=−y1, z=z0).

In the examples of FIG. 4A and FIG. 11A, the optical axis 41 of theoutput splitting/combining device 40 may be parallel to the optical axis31 of the input splitting/combining device 30. In other examples, theoptical axis 41 of the output splitting/combining device 40 may bechanged and may be perpendicular to the optical axis 31 of the inputsplitting/combining device 30; and the one or more output optical fibersmay have one or more locations changed along X direction, such that anoptical isolator of the present disclosure can still operate as anon-reciprocal device only allowing one-way transmission of light.

FIGS. 15-16 show one such example of an isolator 300. In this example,the output optical fiber 20 can be changed from the previous location(x=−x0, z=z0) in FIGS. 6 and 7 to another location (x=−x1, z=z0) inFIGS. 15 and 16 along X direction for outputting. For thisconfiguration, the location value x1 can be given by x1=x0+c1, and c1 isthe amount of change between x1 and x0. The optical axis (41) of theoutput splitting-combining device 40 has a different orientation. Inparticular, the optical axis 41 may be in or parallel to the surface 42of the crystal of the device 40 and can be perpendicular to the opticalaxis (31) of the input device 40. The angle (A41) between the opticalaxis 41 and the edge (43) (e.g., along +X direction) of the surface (42)of the crystal of the device 40 may be 135 degrees. Thus, thebirefringence of the output splitting-combining device 40 in FIGS. 15-16is opposite to that of FIGS. 6-7. While, the configuration of theinput-splitting device 30 is the same for both configurations in FIGS.6-7 and 15-16.

Nevertheless, the isolator 300 allows incident light of an optical beamin a forward light path at the input 10 to pass for output at the output20, but isolates incident light in a backward light path. As shown inFIG. 15, the forward light path in the X-Z plane is as follows. Anincident light beam is input from the input optical fiber 10 (x=x0,z=z0) along the Z direction. The light beam passes the inputsplitting/combining device 30 to cause the splitting of the o light andthe e light in the crystal of the input splitting/combining device 30.That is, one incident beam is split into two linear polarized lightbeams, having a first linear polarized light beam, e light, polarized ina direction in X-Z plane and perpendicular to the light propagationdirection indicated by a double-headed arrow 35, and a second linearpolarized light beam, o light, polarized in the Y direction indicated bya dot 36. The beams enter the input optical rotation device 50, and thepolarization directions of the two linear polarized light beams arerotated clockwise by 0 degree, i.e., being not rotated by the inputoptical rotation device 50, e.g., viewing along −Z direction.

From the rotation device 50, the beams enter the lens 70, where beamcollimation and focusing are performed. As the beams pass themagneto-optical crystal 81 in the Faraday rotator 80 (from an S pole),the polarization directions of the two linear polarized light beams arerotated counter-clockwise by 22.5 degrees, e.g., viewing along −Zdirection. Passing from the rotator 80, the beams are focused onto thereflection surface 91 of the reflector 90. In the example of FIG. 15,the Faraday rotator 80 can be oriented or configured, such that as thebeams pass the magneto-optical crystal 81 from the lens 70, the beamspass the magneto-optical crystal 81 from an S pole.

At the reflector 90, the beams are reflected by the reflection surface91 and return to or reach the magneto-optical crystal 81 in the Faradayrotator 80, and, accordingly, the polarization directions of the twolinear polarized light beams are rotated counter-clockwise by 22.5degrees, e.g., viewing along −Z direction. Passing from the rotator 80,the beams enter the output optical rotation device 60, and thepolarization directions of the two linear polarized light beams arerotated clockwise by 45 degrees, e.g., viewing along −Z direction. Atthis point, the total rotation angle of each of the two linear polarizedlight beams is 0 degrees clockwise, e.g., viewing along −Z direction.Therefore, the beams can be combined by further entering the outputsplitting/combining device 40. In the example of FIG. 15, as the opticalaxis 41 of the output splitting/combining device 40 is perpendicular tothe optical axis 31 of the input splitting/combining device 30, the beamenters the output optical fiber 20 at the location (x=−x1, z=z0) foroutputting.

In contrast to the forward light path of FIG. 15, the isolator 300 asshown in FIG. 16 isolates incident light of an optical beam in abackward light path at the output 20 from being output at the input 10.The backward isolation light path in the X-Z plane is as follows. Anincident light beam is input from the output optical fiber 20 (x=−x1,z=z0) along the Z direction. The light beam passes the outputsplitting/combining device 40, which splits of the o light and the elight in the crystal of the output splitting/combining device 40. Thatis, one incident beam is split into two linear polarized light beams,having a first linear polarized light beam, e light, polarized in adirection perpendicular to the light propagation direction and in X-Zplane, as indicated by a double-headed arrow, and a second linearpolarized light beam, o light polarized in the Y direction indicated bya dot, in the crystal of the output splitting/combining device 40.

From the splitting/combining device 40, the beams enter the outputoptical rotation device 60, and the polarization directions of the twolinear polarized light beams are rotated counterclockwise by 45 degrees,e.g., viewing along −Z direction. From the rotating device 60, the beamsenter the lens 70, and beam collimation and focusing are performed. Asthe beams pass the magneto-optical crystal 81 in the Faraday rotator 80,the polarization directions of the two linear polarized light beams arerotated counterclockwise by 22.5 degrees, e.g., viewing along −Zdirection.

At the reflector 90, the beams are focused onto the reflection surface91 of the reflector 90. The beams are reflected by the reflectionsurface 91 and return to the magneto-optical crystal 81 in the Faradayrotator 80, and, accordingly, the polarization directions of the twolinear polarized light beams are rotated counterclockwise by 22.5degrees, e.g., viewing along −Z direction. Further, the beams enter theinput optical rotation device 50, and the polarization directions of thetwo linear polarized light beams are rotated clockwise by 0 degree,i.e., not being rotated by the input optical rotation device 50, e.g.,viewing along −Z direction. At this point, the total rotation angle ofeach of the two linear polarized light beams is 90 degree. Therefore,the beams are not combined after further entering the inputsplitting/combining device 30. Instead, the input splitting/combiningdevice 30 further displaces the e-light relative to the o-light.Accordingly, the input optical fiber 10 (x=x0, z=z0) has no light beamto output.

The present invention provides an optical isolator used in the field ofoptical communications, with optical fibers arranged on one single side.The optical isolator with optical fibers arranged on one single side mayinclude an input optical fiber, an output optical fiber, an inputsplitting/combining device, an output splitting/combining device, aninput optical rotation device, an output optical rotation device, alens, a Faraday rotator, and a reflector. A scheme of a light pathhaving a reflector is adopted in the present disclosure, andaccordingly, the optical isolator with optical fibers arranged on onesingle side only needs to use one collimator, and the input and theoutput are on the same side of the device. Thus, smaller size, lowercost, and simpler assembly process thereof may be obtained in a opticalisolator consistent with the present disclosure, as compared to opticalisolators that have optical fibers arranged on two sides. Further, thesplitting/combining devices may be fixed on end surfaces of aninput/output optical fibers, the volume of splitting/combining devicesrequired by the optical isolator with optical fibers arranged on asingle side may be reduced, and a more compact structure and lowermaterial cost may be obtained.

It should be noted that variations and modifications to the embodimentsdisclosed herein are possible. Those of ordinary skills in the artshould be aware that various modifications made to the form and detailsof the present disclosure without departing from the spirit and range ofthe present disclosure shall all fall within the protection scope of thepresent invention.

The present disclosure may be embodied in other specific forms withoutdeparting from its spirit or essential characteristics. The describedembodiments are to be considered in all respects only as illustrativeand not restrictive.

1. An optical isolator device for one-way transmission of an opticalbeam, the isolator comprising: an input, for the optical beam, having:an input birefringent device, and an input rotation device disposed inoptical communication with the input birefringent device; an output, forthe optical beam, having: an output birefringent device, and an outputrotation device disposed in optical communication with the outputbirefringent device; an intermediate rotation device disposed in opticalcommunication with the input and output rotation devices; a reflectordisposed in optical communication with the intermediate rotation deviceand configured to reflect the optical beam incident thereto.
 2. Thedevice of claim 1, wherein each of the birefringent devices isconfigured to displace extraordinary light (e-light) relative toordinary light (o-light) of the optical beam incident thereto.
 3. Thedevice of claim 1, wherein each of the rotation devices is configured torotate polarized light of the optical beam incident thereto.
 4. Thedevice of claim 1, wherein the input comprises one or more input fibersdisposed in optical communication with the input birefringent device;and wherein the output comprises one or more output fibers disposed inoptical communication with the output birefringent device.
 5. The deviceof claim 4, comprising a dual-fiber head having a first input fiber ofthe one or more input fibers and a first output fiber of the one or moreoutput fibers disposed therein, the first output fiber and the firstinput fiber being symmetric with respect to a central axis of thedual-fiber head.
 6. The device of claim 4, wherein: the inputbirefringent device is fixed on an end face of the one or more inputoptical fibers; and the output birefringent device is fixed on an endface of the one or more output optical fibers.
 7. The device of claim 1,wherein: the input rotation device is fixed on the input birefringentdevice; and the output rotation device is fixed on the outputbirefringent device.
 8. The device of claim 1, further comprising a lensdisposed in optical communication between the intermediate rotationdevice and the input and output rotation devices.
 9. The device of claim8, wherein the lens comprises: a first focus plane on a first side ofthe lens; and a second focus plane on a second side of the lens.
 10. Thedevice of claim 9, wherein an end face of one or more input opticalfibers for the input and an end face of one or more output opticalfibers for the output are disposed on the first focus plane of the lens.11. The device of claim 1, wherein: the input is configured to passincident light of the optical beam at the input to the inputbirefringent device; the input birefringent device is configured tosplit first and second polarized light beams from the incident light; acombination of the input rotation device, the intermediate rotationdevice, and the output rotation device is configured to rotate apolarization direction of each of the first and second polarized lightbeams by 90 degrees; and the output birefringent device is configured tocombine the first and second polarized light beams incident thereto fromthe output rotation device into output light for the output.
 12. Thedevice of claim 11, wherein: the input rotation device is configured torotate the polarization direction of each of the first and secondpolarized light beams by zero degree; the intermediate rotation deviceis configured to rotate the polarization direction of each of the firstand second polarized light beams by 45 degrees in a first rotation; andthe output rotation device is configured to rotate the polarizationdirection of each of the first and second polarized light beams by 45degrees in the first rotation.
 13. (canceled)
 14. The device of claim12, wherein the intermediate rotation device is configured to rotate thepolarization direction of each of the first and second polarized lightbeams incident thereto in a prorogation direction from the input by 22.5degrees in the first rotation and is configurated to rotate thepolarization direction of each of the first and second polarized lightbeams incident therefrom in a reflected direction from the reflector by22.5 degrees in the first rotation.
 15. The device of claim 11, whereina splitting direction of the first and second polarized light beams isperpendicular to a beam propagation direction of the incident light beamand is parallel to a direction of relative displacement between theinput and the output.
 16. The device of claim 1, wherein: the output isconfigured to pass incident light of the optical beam at the output tothe output birefringent device; the output birefringent device isconfigured to split first and second polarized light beams from theincident light; a combination of the output optical rotation device, theintermediate rotation device, and the input rotation device isconfigured to rotate a polarization direction of each of the first andsecond polarized light beams by zero degree; the input birefringentdevice is configured to split the first and second polarized light beamsincident thereto from the input rotation device further in isolationfrom the input.
 17. The device of claim 16, wherein: the output rotationdevice is configured to rotate the polarization direction of each of thefirst and second polarized light beams by 45 degrees in a firstrotation; the intermediate rotation device is configured to rotate thepolarization direction of each of the first and second polarized lightbeams by 45 degrees in a second rotation opposite the first rotation;and the input rotation device is configured to rotate the polarizationdirection of each of the first and second polarized light beams by zerodegree.
 18. The device of claim 1, wherein: the input birefringentdevice include a birefringent crystal having a first optical axis; theoutput birefringent device include a birefringent crystal having asecond optical axis. 19-20. (canceled)
 21. The device of claim 1,wherein the intermediate rotation device comprises a Faraday rotatorhaving a magneto-optical crystal and a magnetic ring disposed at leastpartially enclosing the magneto-optical crystal.
 22. (canceled)
 23. Thedevice of claim 21, wherein the magnetic ring comprises a permanentmagnet configured to provide a saturated magnetic field strength of themagneto-optical crystals, causing the magneto-optical crystals to havefixed rotation of a polarization direction of linear polarized light.24. The device of claim 1, wherein at least one of the input, output,and birefringent devices comprises a displacement-type birefringentcrystal and is configured to split/combine o-light and e-light insidethe birefringent crystal.
 25. The device of claim 1, wherein the inputrotation device and the output rotation device each comprises a ½wavelength (X) phase delay-type crystalline quartz waveplate configuredto rotate a polarization direction of linear polarized light.
 26. Anoptical isolator device for one-way transmission of light, the isolatorcomprising: first and second input optical fibers; an inputsplitting-combining device disposed in optical communication with thefirst and second input optical fiber; an input optical rotation devicedisposed in optical communication with the input splitting-combiningdevice; a lens in optical communication with the input optical rotationdevice; a rotator disposed in optical communication with the lens andconfigured to rotate a polarization direction of a light beam; areflector configured to receive one or more light beams from the rotatorand reflect the one or more light beams to the rotator; an outputoptical rotation device disposed in optical communication with the lens;an output splitting-combining device disposed in optical communicationwith output optical rotation device; and first and second output opticalfibers disposed in optical communication with the outputsplitting-combining device; wherein: the first and second input opticalfibers and the first and second output optical fibers are arranged on asame side of the reflector. 27-30. (canceled)